ES2356227T5 - Security element with micro and macrostructures - Google Patents

Abstract

A security element which is difficult to copy includes a layer composite which has microscopically fine, optically effective structures of a surface pattern, which are embedded between two layers of the layer composite. In a plane of the surface pattern, which is defined by co-ordinate axes x and y, the optically effective structures are shaped into an interface between the layers in surface portions of a holographically non-copyable security feature. In at least one surface portion the optically effective structure (9) is a diffraction structure formed by additive superimposition of a macroscopic superimposition function (M) with a microscopically fine relief profile (R). Both the relief profile (R), the superimposition function (M) and also the diffraction structure are functions of the co-ordinates x and y. The relief profile (R) is a light-diffractive or light-scattering optically effective structure and, following the superimposition function (M), retains the predetermined profile height. The superimposition function (M) is at least portion-wise steady and is not a periodic triangular or rectangular function. In comparison with the relief profile (R) the superimposition function (M) changes slowly. Upon tilting and rotation of the layer composite the observer sees on the illuminated surface portions light, continuously moving strips which are dependent on the viewing direction.

Description

E03714917

09-24-2014

DESCRIPTION

Security element with micro and macrostructures

The present invention relates to a security element according to the preamble of claim 1.

Safety elements of this type are composed of a thin laminated composite material of plastic, with at least one embossed structure of the diffraction structure group, light scattering structures and flat reflective surfaces being included in the stratified composite material. Security elements

10 cut from the thin stratified composite material are glued on objects to certify the authenticity of the objects.

The construction of the thin stratified composite material and the materials used for this are described for example in US 4,856,857. From GB 2 129 739 A it is also known to apply the laminated composite material with the aid of a support sheet on the object.

From EP 0 429 782 B1 a prior art arrangement is known. The security element glued in a document has an optically variable surface pattern, known from EP 0 105 099 A1 of mosaic-shaped surface portions with known diffraction structures. So that a forged document cannot be provided with a false security element cut from an authentic document or detached from an authentic document to simulate apparent authenticity without clear marks, security profiles are printed on the security element and adjacent parts of the document . The authentic document is distinguished by security profiles that extend without rupture by the security element in adjacent parts of the document. Printing security profiles alters the

25 optically variable surface pattern identification. Especially varies the position of the wedge on the security element between copies of the document.

It is also known to provide security elements with features that hinder or make a counterfeit or reproduction with usual holographic means completely impossible. For example, EP 30 0 360 969 A1 and WO 99/38038 describe arrangements of asymmetric optical grilles. The surface elements have grilles that, used under different azimuthal angles, form a pattern modulated in the luminosity in the surface pattern of the security element. In a holographic copy the modulated pattern is not reflected in the luminosity. If the grid structures, such as described in WO 98/26373, are shorter than the wavelength of the light used for reproduction, such submicroscopic structures are no longer detected and

35 therefore in the copy they are not reflected in the same way.

WO 01/80175 A1 describes a diffractor surface pattern that is configured as a visible mosaic composed of surface parts in a plastic laminate. At least on a surface part a "zero order microstructure" is molded with a modulated grid profile, whose spatial frequency f

40 multiplied by a predetermined limit wavelength of the visible spectrum results in a product greater than or equal to one.

The protective device against holographic reproduction described in EP 0 360 969 A1, WO 98/26373 and WO 99/38038 mentioned by way of example is acquired with technical production difficulties.

The invention is based on the objective of achieving a new, economical security element that must have a high resistance against counterfeiting attempts, for example by means of a holographic reproduction procedure.

This objective is solved by a security element according to claim 1.

Advantageous configurations of the invention result from the dependent claims.

Show

Figure 1 a security element in cross section, Figure 2 the security element in plan view, Figure 3 the reflection and diffraction in a grid, Figure 4 the illumination and observation of the security element,

60 Figure 5 the reflection and diffraction in a diffraction structure, Figures 6 the safety feature at different angles of inclination, Figure 7 an overlapping function and the diffraction structure in cross section, Figures 8 the orientation of the element of safety by means of identification marks figure 9 a local inclination angle of the overlay function,

65 figures 10 the orientation of the security element by means of color contrast in the

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safety feature, figure 11 the diffraction structure with symmetric overlay function, figures 12 the safety feature with color alteration and figure 13 an asymmetric overlay function.

In Fig. 1, 1 means a laminated composite material, 2 a safety element, 3 a substrate, 4 a surface layer, 5 a molded layer, 6 a protective layer, 7 an adhesive layer, 8 a reflective boundary surface, 9 a optically active structure and a transparent point on the reflective boundary surface 8. The laminated composite material 1 is composed of several layers of different plastic layers applied one on top of the other, on a support sheet not shown in this case and normally comprises in the indicated order the surface layer 4, the molded layer 5, the protective layer 6 and the adhesive layer 7. The surface layer 4 and the molded layer 5 are transparent to the incident light 11. If the protective layer is also transparent 6 and the adhesive layer 7, signals placed on the surface of the substrate 3 can be identified by the transparent dots 10. The support sheet itself serves in one embodiment surface layer 4, in another embodiment, a backing sheet serves to apply the thin stratified composite 1 on the substrate 3 and then is removed from the stratified composite 1 as described for example in GB 2 129 739 A mentioned above .

The common contact surface between the molded layer 5 and the protective layer 6 is the boundary surface 8. In the molded layer 5, the optically active structures 9 with a height of HST structure of an optically variable pattern are molded. Since the protective layer 6 fills the valleys of the optically active structures 9, the boundary surface 8 has the shape of the optically active structures 9. In order to obtain a high activity of the optically active structures 9, a metal coating is provided with the boundary surface 8, preferably of the elements of table 5 of US 4,856,857 mentioned above, especially aluminum, silver, gold, copper, chrome , tantalum and so on, which as a reflection layer separates the molded layer 5 and the protective layer 6. The electrical conductivity of the metallic coating causes a high reflection capacity of the visible incident light 11 on the boundary surface 8. However, in addition to the coating One or more layers of one of the inorganic, transparent, known dielectric compounds that are mentioned, for example, in Tables 1 and 4 of US 4,856,857 mentioned above are also suitable, or the reflection layer has a multiple interference layer. layers, such as a combination of two-layer dielectric metal-compound or a combination of meta l-dielectric-metal compound. The reflection layer is structured in one embodiment, that is to say it covers the boundary surface 8 only partially and in predetermined areas of the boundary surface 8.

The laminated composite 1 is produced as a plastic sheet in the form of a long sheet with a plurality of copies arranged side by side of the optically variable pattern. The security elements 2 are cut, for example, from the sheet and by means of the adhesive layer 7 they are joined with a substrate 3. The substrate 3, in most cases in the form of a document, a banknote, a Bank card, an identification card or other important or valuable object, is provided with security element 2 to certify the authenticity of the object.

Figure 2 shows a section of the substrate 3 with the security element 2. In the middle of the surface layer 4 (figure 1) and the molded layer 5 (figure 1) a surface pattern 12 can be seen. The surface pattern 12 It is in a plane defined by the x, y coordinate axes, and contains a safety feature 16 of at least one surface part 13, 14, 15 that can be well identified with the naked eye on the contour, that is, the dimensions of The surface part are at least in a direction greater than 0.4 mm. Security feature 16 is doubly framed for representation in the drawing of Figure 2. In another embodiment, security feature 16 is surrounded by a mosaic of surface elements 17 to 19 of the mosaic described in EP 0 105 099 A1 mentioned above. On the surface parts 13 to 15 and, if necessary, on the surface elements 17 to 19, the optically active structures 9 are molded (Figure 1), such as microscopically fine diffraction gratings, relief structures that scatter light, microscopically thin or surfaces flat reflectors on the boundary surface 8 (figure 1).

Figure 3 describes how the light 11 that strikes the boundary surface 8 (figure 1) is reflected and diffracted by default through the optically active structure 9. The incident light 11 penetrates the diffraction plane 20, which is perpendicular to the surface of the laminated composite 1 with the security element 2 (Figure 1) and contains a surface normal 21, on the optically active structure 9 in the stratified composite material 1. The incident light 11 is a parallel beam of light rays and includes the angle of incidence  with the normal surface 21. If the optically active structure 9 is a flat reflective surface parallel to the surface of the stratified composite material 1, the surface normal 21 and the direction of the reflected light 22 form the arm of the reflection angle , where  = -. In the event that the optically active structure 9 is one of the known grids, the grid deflects the incident light 11 in different diffraction orders 23 to 25 determined by the spatial frequency f of the grid, assuming that the grid vector described the grid is in the diffraction plane 20. The wavelengths  contained in the incident light 11 deviate under the predetermined angles in the different diffraction orders 23 to 25. For example, the grid deflects the violet light ( = 380 nm) simultaneously as ray 26 in the order of diffraction 23 plus 1, such as ray

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27 in the order of diffraction 24 minus 1 and as ray 28 in the order of diffraction 25 minus 2. Parts of light with longer wavelengths incidente of incident light 11 emerge in directions with diffraction angles greater than normal of surface 21, for example the red light, ( = 700 nm) in the directions designated with the arrows 29, 30, 31. The polychromatic incident light 11 expands due to the diffraction in the grid in the light rays of the different wavelengths incidente of the incident light 11, ie the visible part of the spectrum extends in the area between the violet light ray (arrow 26 or 27 or 28) and the red light ray (arrow 29 or 30 or 31 ) in each diffraction order 23 or 24 or 25. The diffracted light in the zero diffraction order is the light 22 reflected under the angle of incidence .

Figure 4 shows a diffraction grating 32 molded in the surface elements 17 (Figure 2) to 19 (Figure 2), whose microscopically thin profile R (x, y) has for example a cross section of the periodic, sinusoidal profile with constant profile height h and with the spatial frequency f. The determined relief of the diffraction grating 32 establishes an average surface 33 arranged parallel to the surface layer 4. The incident light 11 parallel passes through the surface layer 4 and the molded layer 5 and is diverted to the optically active structure 9 (Figure 1) of the diffraction grating 32. The parallel diffracted rays of light 34 of the wavelength  leave the security element 2 in the direction of the gaze of an observer 35, which in the case of the pattern lighting of surface 12 (figure 2) with the light 11 incident in a parallel manner, spot the colored surface elements 17, 18, 19 that shine brightly.

In Fig. 5, the diffraction plane 20 is in the drawing plane. At least one of the surface parts 13 (figure 2) to 15 (figure 2) of the safety feature 16 (figure 2) a diffraction structure S (x, y) is molded, whose average surface 33 is inclined from arched or locally the surface of the stratified composite material 1. The diffraction structure S (x, y) is a function of the x and y coordinates in the plane of the surface pattern 12 parallel to the surface of the stratified composite 1 (Figure 2) , where the surface parts 13, 14 (Figure 2), 15 are located. At each point P (x, y), the diffraction structure S (x, y) determines a distance z parallel to the normal surface 21 with respect to the plane of the surface pattern 12. Generally described, the diffraction structure S (x, y) is the sum of the relief profile R (x, y) (Figure 4) of the diffraction grating 32 ( Figure 4) and an overlapping function M (x, y) uniquely defined, of the average surface 33, where S (x, y) = R (x, y) + M (x, y). For example, the relief profile R (x, y) generates the periodic diffraction grating 32 with the profile of one of the rectangular, asymmetric or symmetrical, or sinusoidal sawtooth shapes.

In another embodiment, the microscopically thin profile R (x, y) of the diffraction structure S (x, y) is a matte structure instead of the periodic diffraction grating 32. The matte structure is a stochastic, microscopically thin structure with a predetermined diffusion characteristic for the incident light 11, in the case of an anisotropic matte structure instead of the grid vector being a preferred direction. The matt structures diffuse the incident light perpendicularly in a diffusion cone with a predetermined opening angle by means of the diffusion capacity of the matte structure and with the direction of the light 22 reflected as the axis of the cone. The intensity of the diffusion light is the maximum for example in the axis of the cone and decreases with increasing distance from the axis of the cone, and an observer can still identify the deflected light in the direction of the lines of the cone layer of diffusion. The cross section of the diffusion cone perpendicular to the axis of the cone is symmetrical in rotation in the case of a matt structure called in this case "isotropic". If the cross-section in the preferred direction on the contrary is compressed, that is, it is elliptically deformed with the short main axis of the ellipse parallel to the preferred direction, the matte structure is here called "anisotropic".

Due to the additive or subtractive overlap, the profile height h (Figure 4) of the relief profile R (x, y) is not modified in the area of the overlay function M (x, y), that is the profile in relief R (x; y) follows the function of superposition M (x, y). The overlap function M (x, y) defined in a unique way can be at least partially differentiated and is curved at least in partial areas, that is ∆M (x, y) = 0, periodic or aperiodic and is not a rectangular or periodic triangular. The periodic overlapping functions M (x, y) have a spatial frequency F of at most 20 lines / mm. For good visibility, the joint segments between two adjacent extreme values of the overlapping functions M (x, y) are at least 0.025 mm long. The preferred values for the spatial frequency F are limited to a maximum of 10 lines / mm and the preferred values for the distance of the adjacent extreme values amount to at least 0.05 mm. Therefore, the overlapping function M (x, y) varies as a macroscopic function in the continuous area slowly compared to the relief profile R (x, y).

A section line projected on the plane of the surface pattern 12 (figure 2) of the diffraction plane 20 with the middle plane 33 establishes a mark 36 (figure 2). The overlapping function M (x, y) presents at each point P (x, y) in the joining segments that are parallel to the mark 36 with continuous sections a gradient 38, grad (M (x, y)). In general, with the gradient 38 the components of the grad (M (x, y)) in the diffraction plane 20 are considered, since the observer 35 establishes the optically active diffraction plane 20. The diffraction grating 32 has a predetermined inclination γ at each point of the surface part 13, 14, 15 by the gradient 38 of the overlapping function M (x, y).

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The deformation of the middle surface 33 causes a new advantageous optical effect. This effect is clarified by the diffraction behavior at penetration points A, B, C of the normal surface 21 and the normal 21 ', 21 "on the average surface 33, for example along the mark 36. The refraction of the incident light 11, of the reflected light 22 and of the light rays 34 diffracted on the boundary surface of the stratified composite material 1 is not represented for reasons of simplicity in the drawing of Figure 5 and is not taken into account in the following calculations: At each penetration point A, B, C, the inclination γ is determined by gradient 38. Normal 21 'and 21 ", of the grid vector of the diffraction grating 32 (figure 4) and a direction of observation 39 of the observer 35 are in the diffraction plane 20. Corresponding to the angle of inclination γ, the angle of incidence  is modified (figure 3), comprising the normal 21, 21 ', 21 "plotted by points and light 11 white inc idente in parallel. This also modifies the wavelength  of the diffracted light rays 34 deflected in a predetermined observation direction 39 with respect to the observer 35. If the normal 21 'is not inclined from the observer 35, the wavelength  of the diffracted light rays 34 is greater than if the normal 21 "bends with respect to the observer 35. In the example shown for the illustration, the diffracted light rays 34 in the area of the penetration point A present the observer 35 with a color red ( = 700 nm) The light rays 34 diffracted in the area of the penetration point B are yellowish green ( = 550 nm) and the light rays 34 diffracted in the area of the penetration point C have a blue color ( = 400 nm) Since, in the example shown, the inclination  is continuously modified through the curvature of the average surface 33, the observer 35 can see along the mark 36 the entire visible spectrum in the pair surface te 13, 14, 15, the color bands of the spectrum extending on the surface part 13, 14, 15 perpendicular to the mark 36. So that the observer 35 can identify the color bands of the spectrum 35 at a 30 cm apart, must be selected for the distance between penetration points A and C at least 2 mm in length or more. Outside the visible spectrum, the surface of the surface part 13, 14, 15 has a gray color of low light intensity. In turning the stratified composite material 1 around a turning axis 41 perpendicular to the plane of the drawing of Figure 5, the angle of incidence  is modified. The visible color bands of the spectrum move in the area of the overlapping function M (x, y) continuously along the mark 36. In the case of a flip, for example in the direction of the needles of the clock around the turning axis 41, of the stratified composite material 1 the color of the light beam 34 diffracted at the point of penetration A is modified to a yellowish green color, the color of the light ray 34 diffracted at the point of penetration B a a blue color and the color of the light ray 34 diffracted at the point of penetration C to a violet color. The observer considers the modification of the colors of the diffracted ray of light 34 as the displacement of the color bands continuously through the surface part 13, 14, 15.

This consideration is applicable for each diffraction order. How many bands of color of how many diffraction orders the observer 35 simultaneously sees on the surface part 13, 14, 15, depends on the spatial frequency of the diffraction grating 32 and the number of periods and the amplitude of the overlay function M (x, y) within the surface part 13, 14, 15.

In another embodiment, in case one of the matte structures is used instead of the diffraction grating 32, the observer 35 sees in the direction of the light 22 reflected only a light off-white gray band instead of the color bands . The light whitish gray band moves with the flip as the color bands continuously across the surface of the surface part 13, 14, 15. Then, unlike the color bands, the light whitish gray band also it can be seen by the observer 35 depending on the dispersion capacity of the matte structure, when its diffraction direction 39 is oblique with respect to the diffraction plane 20. Therefore, it is then considered as "band 40" (figure 6a) both color bands of an order of diffraction 23, 24, 25 as the light whitish gray band generated by the matt structure.

In figure 6a, the observer 35 (figure 5) can slightly identify the displacement of the band, when there is a reference in the safety feature 16. Identification marks 37 (figure 2) arranged in the surface part 13 serve as reference. , 14, 15, for example in the middle surface part 14, and / or a predetermined boundary form of the surface part 13, 14, 15. Advantageously, the reference establishes a predetermined observation condition, which can be adjusted by of the turning of the laminated composite material 1 (figure 1) such that the band 40 is placed by default in front of the reference. In the area of the identification marks 37, the optically active structure 9 (figure 1) of the boundary surface 8 (figure 1) is designed with advantage as an optically active structure 9, a diffraction structure, a reflecting surface or an embossed structure that scatters light, which is molded with the replication of surface pattern 12 in the register of surface portions 13, 14, 15. However, a light absorbing impression on safety feature 16 can also be used as a reference for movement of the band or identification mark 37 is generated by means of the structured reflection layer.

In another embodiment of the safety feature 16 according to FIGS. 6, the adjacent surface portions 13 and 15, which include the middle surface portion 14 on both sides, serve as reciprocal reference. The adjacent surface portions 13 and 15 both have a diffraction structure S * (x, y). The diffraction structure S * (x, y), unlike the diffraction structure S (x, y), is the difference between the RM of the relief function R (x, y) and the superposition function M ( x, y), that is S * (x, y) = R (x, y) - M (x, y). The color bands generated by the diffraction structure S * (x, y) have an inverse color gradient compared to the color bands of

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the diffraction structure S (x, y), as indicated in the drawing of figure 6a by means of a thick longitudinal edge of the band 40. For a good visibility of the optical effect without auxiliary means, the safety feature 16 it presents along the coordinate axis and the mark 36 a dimension of at least 5 mm, preferably more than 10 mm. The dimensions along the x-axis coordinate amount to more than 0.25 mm, but preferably at least 1 mm.

In the embodiment of the safety feature 16 according to Figures 6a to 6c, the oval surface part 14 has the diffraction structure S (y) dependent only on the y-coordinate, while the surface parts 13 and 15 with the structure diffraction S * (y) dependent only on the coordinate and extend on both sides of the surface part 14 along the coordinate y. The superposition function is M (y) = 0.5 • y2 • K, where K is the curvature of the middle surface 33. Gradient 38 (figure 5) and the grid vector of the diffraction grating 32 (figure 4 ) or the preferred direction of the "anisotropic" matte structure are aligned parallel or antiparallel in the direction of the y coordinate.

In general, the azimuth  of the grid vector or the preferred direction of the matte structure refers to a gradient plane, which is determined by gradient 38 and the normal surface 21. The preferred values of the azimuth  are 0 ° and 90 °. In this regard, deviations in the azimuth angle of the grid vector or the preferred direction of  =  20 ° in the preferred value are allowed, to observe in this area the grid vector or the preferred direction essentially as parallel or perpendicular to the gradient plane. The azimuth  is not limited to the preferred values mentioned.

The smaller the curvature K, the greater the speed of movement of the band 40 in the direction of the arrows not indicated in the drawing of Figures 6a and 6c per unit of rotation angle around the axis of rotation

41. The band 40 is shown in the drawing of Figures 6a to 6c in a narrow manner, to clearly represent the effect of movement. The width of the bands 40 in the direction of the unmarked arrows depends on the diffraction structure S (y). Especially, in the case of the color bands, the spectral color gradient extends through a thicker part of the surface part 13, 14, 15, so that the movement of the bands 40 due to the displacement of a section in the visible spectrum, for example of the red band.

Figure 6b shows the safety feature 16 after a rotation around the turning axis 41 at a predetermined turning angle, in which the band 40 of both outer surface parts 13, 15 and the middle surface part 14 meet at a line parallel to the turning axis 41. This predetermined turning angle is determined by the selection of the overlay structure M (x, y). In one embodiment of the security element 2 (figure 2) only a predetermined pattern should be observed in the surface pattern 12 (figure 2), when in the safety feature 16 the band or bands 40 occupy a predetermined area, that is when the observer 35 observes the safety element 2 under the observation conditions determined by the predetermined turning angle.

In Figure 6c, after an additional rotation around the turning axis 41, the bands are moved again separately in the safety feature 16, as indicated by the arrow not indicated in Figure 6c.

Logically, an adjacent arrangement of the middle surface part 14 and one of the two surface parts 13, 15 are aligned to obtain the safety feature 16 in another embodiment.

Figure 7 shows a cross-section along the mark 36 (figure 2) by means of the laminated composite material 1 for example in the area of the surface part 14 (figure 2). So that the stratified composite material 1 that is too thick cannot be produced or used, and the height of the structure HSt (Figure 1) of the diffraction structure S (x; y) is limited. In the non-scale drawing of Figure 7, the overlapping function M (y) = 0.5 • y2 • K is shown exclusively in section on the left of the coordinate axis z, in which the height of the laminated composite 1. At each point P (x, y) of the surface part 14 the value z = M (x, y) is limited to a predetermined path H = z1 -z0. As soon as you have achieved the overlapping function M (y) at one of the points P1, P2, ..., Pn the value z1 = M (Pj) for j = 1, 2, ..., n, appears in the function of superposition M (y) a discontinuous site in which the value of the superposition function M (y) on the separate side of the point P0 is respectively reduced to approximately the value H at the height z0, that is the value used of the function of superposition M (x; y) on the diffraction structure S (x; y) is the function value

Z = {M (x; y) + C (x; y)} H-C (x; y) path module.

The function C (x; y) is limited in this respect quantitatively in a range of values, for example half of the HST structure height value. The discontinuous sites of the function {M (x; y) + C (x; y)} path module H - C (x; y) generated for technical reasons are not listed as extreme values of the overlapping function M (x; y ). Similarly, in certain embodiments, the values of the path H may be locally small. In an embodiment of the diffraction structure S (x, y), the path H which varies locally is determined because the distance between two successive discontinuous sites Pn does not exceed a predetermined value in the range of from 40 hastam to

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300 m.

On the surface portions 13 (Figure 2), 14, 15 (Figure 2) the diffraction structure S (x, y) is extended on both sides of the coordinate axis z and not only on the right side of the coordinate axis z, as shown in the drawing of figure 7. Due to the overlap, the structure height HSt is the sum of the path H and the profile height h (figure 4) and is equal to the value of the diffraction structure S ( x, y) at the point P (x; y). The structure height HSt is advantageously less than 40 m, with preferred values of the structure height HSt <5 m. The path H of the overlapping function M (x, y) is limited to less than 30 µm and is preferably in the range of H = 0.5 µm to H = 4 µm. The matt structures have fine relief elements of microscopic scale, which determine the dispersibility and can be described only with statistical parameters, such as for example the average roughness value Ra, the correlation length lc and so on, the values being found for the average roughness value Ra in the range of 200 nm to 5 µm with preferred values from Ra = 150 nm to Ra = 1.5 µm, while the correlation lengths lc are at least in the range of from 300 nm to 300 µm, preferably between lc = 500 nm and lc = 100 µm. In the case of "isotropic" matt structures, the statistical parameters depend on a preferred direction, while in the case of "anisotropic" matt structures, the relief elements are aligned with the correlation length lc perpendicularly with respect to The preferred address. The profile height h of the diffraction grating 32 (Figure 4) has a value of the interval of h = 0.05 mah = 5 m, the preferred values being in the narrowest range of from h = 0.6  0.5 m. The spatial frequency f of the diffraction grating 32 is selected from the range of f = 300 lines / mm to 3300 lines / mm. From approximately F = 2400 lines / mm the diffracted light 34 can be observed (figure 5) only in the order of zero diffraction, that is in the direction of the reflected light 22 (figure 5).

Additional examples of the overlay function M (x, y) are:

M (x, y) = 0.5 • (x2 + y2) • K, M (x, y) = a • {1 + sin (2πFx • x) • sen (2πFy • y)},

M (x, y) = a • x1.5 + b • x, M (x, y) = a • {1 + sin (2πFy • y)}, where Fx or Fy is the spatial frequency F of the superposition function M (x, y) in the direction of the xo y coordinate axis. In another embodiment of the safety feature 16, the overlapping function M (x, y) is periodically composed of a predetermined section of another function and has one or more periods along the mark 36.

In Figure 8a, the overlapping function M (x, y) = 0.5 • (x2 + y2) • K, ie a spherical shell, and the relief structure R (x, y), that is to say a structure "Isotropic" matte, form the diffraction structure S (x, y) (Figure 7) in for example the surface part 14 drawn in a circular shape. The observer 35 (figure 5) identifies, in case of daylight, corresponding to the direction of observation 39 (figure 5) a whitish gray spot 42, clear in front of a dark gray background 43, the position of the spot 42 depending on the surface part 14 with respect to the identification mark 37 and the contrast between the stain 42 and the bottom 43 of the observation direction 39. The extent of the stain 42 is determined by the dispersibility of the matte structure and the curvature of the superposition function M (x, y). The safety element 2 (figure 2) is aligned in the predetermined observation direction 39 for example by turning around the turning axis 41 (figure 5) and / or rotating around the normal surface 21 (figure 5) of the composite material laminated 1 (figure 5) as in figure 8b in such a way that the stain 42 is inside the identification mark 37, which for example is arranged in the middle of the surface part 14 drawn in a circular shape.

Figure 9 shows the light diffraction action of the diffraction structure S (x, y) (figure 7) in the diffraction plane 20. The relief structure R (x, y) (figure 4) is the grid of diffraction 32 (figure 4) with a profile for example sinusoidal and with a spatial frequency f less than 2400 lines / mm. The grid vector of the relief structure R (x, y) is in the diffraction plane 20. The overlapping function M (x, y) on the surface part 13 (figure 2), 14 (figure 2) , 15 (figure 2) of the safety feature 16 is determined by the action of the diffraction structure S (x, y), the incident light 11 deflecting perpendicularly in the stratified composite 1 under an observation angle + or - predetermined in the positive diffraction order 23 (figure 3) or in the negative diffraction order 24 (figure 3). In the diffraction plane 20, first rays 44 with the wavelength 1 include the observation angle with the incident light 11 and second rays 45 with the wavelength 2, the observation angle -. The observer 35 (Figure 5) sees the surface part 13, 14, 15 below the angle of observation in the color with the wavelength 1. After a rotation of the laminated composite material 1 in its 180 ° plane, the surface portion 13, 14, 15 appears to the observer 35 under the observation angle - in the color of the wavelength 2. When the average surface 33 has the local inclination  = 0 °, the wavelengths 1 and 2 do not differ. For other values of the local inclination las the wavelengths 1 and 2 differ. The normal 21 ’shown by points on the inclined middle surface 33 includes the angle  with the incident ray 11, where  = - = . The first rays 44 and the normal 21 ’include the diffraction angle 1, the rays 45 and the normal 21’, the diffraction angle 2.

Because k = asen (sin + mk • k • f) and  =  results for the first two diffraction orders 23, 24, that is, for mk =  1, the relationship

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f • (1 + 2) = 2 • sen () • cos () (1)

from which it follows that for predetermined values of the observation angle and the spatial frequency f, the sum of the two wavelengths 1, 2 of the rays 44, 45 is proportional to the cosine of the local inclination angle . Equation (1) must be easily derived for other order numbers m. The order numbers m and the observation angle for a given color that can be observed are determined by the spatial frequency f.

In figures 10a and 10b an embodiment of the safety feature 16 is shown as an example, in which the security element 2 in figure 10a is rotated 180 ° with respect to the security element 2 in figure 10b in its plane. The diffraction plane 20 (figure 9) is represented by its mark 36. In figures 10a and 10b, the safety feature 16 comprises the three surface parts 13, 14, 15 with the diffraction structure S (x, y) = R (x, y) + M (x, y), differentiating the diffraction structures S (x, y) in the three surface parts 13, 14, 15 using the values determined with the help of equation (1) of the local inclinations  of the superposition function M (x, y) and of the spatial frequency f of the relief profile R (x, y). A background field 46 limits at least a surface portion 13, 14, 15 and has the diffraction grating 32 (Figure 4) with the same raised profile R (x, y) and the spatial frequency f inherent in the field of background 46. The grid vector of the relief profile R (x, y) is aligned on the surface portions 13, 14, 15 and in the background field 46 parallel to the mark 36. In the case of perpendicular illumination of the safety element 2 with white light 11 (figure 9), the surface portions 13, 14, 15 and the background field 46 shine in the same color in the safety feature 16 in the orientation of the figure 10a under the angle of observation +, and the safety characteristic 16 seems to shine to the observer 35 (figure 5) without contrast in a uniform color, for example, the first deflected rays 44 (figure 9) have the wavelength 1, for example 680 nm (Red). In the orientation shown in Figure 10b, the entire safety feature 16 is observed under the observation angle -. For example, the first surface part 13 shines in the second rays 45 (Figure 9) of the wavelength 2, for example 2 = 570 nm (yellow), the second surface part 14 in the second rays 45 of the wavelength 3, for example 3 = 510 nm (green) and the third part of surface 15 in the second rays 45 of the wavelength 4, for example 4 = 400 nm (blue). In the background field 46, in which the average surface 33 (figure 9) of the diffraction grating 32 (figure 4) has the inclination  (figure 9) with the value  = 0, the second rays 45 are also by symmetry motifs of the wavelength 1, that is to say the background surface 46 shines again in the color red. The advantage of this embodiment is the striking optical behavior of the security feature 16, namely the visible color contrast under a unique predetermined orientation of the security element 2 that can be modified or disappeared after a 180 ° rotation of the security element 2 around the normal surface 21 (figure 3). Accordingly, security feature 16 serves to establish a predetermined orientation of security element 2 with security feature 16 that cannot be copied in a holographic manner.

Just to simplify, on each surface part 13, 14, 15 a uniform color was acquired as an example, ie a constant inclination inclinación. In general, the surface part 13, 14, 15 has a section of the overlapping function M (x, y), so that the inclination  in the surface part 13, 14, 15 is continuously modified in a Default direction and wavelengths of the second rays 45 come from an interval on both sides of the wavelength k. Instead of the surface portions 13, 14, 15 similarly limited, a plurality of the surface portions 13, 14, 15 arranged in the background field 46 form a logo, a character and so on.

The diffraction structure S (x, y) is configured in a more complicated way in Figure 11. The overlapping function M (x, y) is a periodic, partially continuous, symmetric function whose value varies along the coordinate axis x according to z = M (x, y), while M (x, y) at along the coordinate axis and has a constant z value. The surface part 13, 14 (figure 10), 15 (figure 10) for example rectangular is aligned with its longitudinal side parallel to the x coordinate, and is divided into narrow partial surfaces 47 of width b, whose longitudinal sides are aligned parallel to the coordinate axis and. Each 1 / Fx period of the overlay structure M (x; y) extends across a number t of partial surfaces 47, for example the number t is in the range of values from 5 to 10. The width b does not it should be below 10 m, since otherwise the diffraction structure S (x, y) is very poorly defined on the partial surface 47.

The diffraction structures S (x, y) of the adjacent partial parts 47 differ in the addends, the relief profile R (x, y) and the section assigned to the partial surface 47 of the overlapping function M (x, y ). The relief profile Ri (x, y) of the ith partial surface 47 differs from the two relief profiles Ri + 1 (x, y) and Ri-1 (x, y) of the partial surfaces 47 by at least a grid parameter, such as azimuth, spatial frequency, profile height h (figure 4) and so on. If the spatial frequency Fx or Fy amounts to a maximum of 10 lines / mm but not less than 2.5 lines / mm, observer 35 (Figure 5) can no longer identify on the surface part 13, 14, 15 to simple view no division by the periods of the superposition function M (x, y). The division and configuration of the partial surfaces 47 with the diffraction structure S (x, y) is repeated in each period of the overlapping function M (x, y). In another embodiment of the safety feature 16, the relief profile R (x, y) is continuously modified as a function of the phase angle of the periodic overlapping function M (x, y).

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The diffraction structures S (x, y) represented in Figure 11 are used in the realization of the safety feature 16 represented in Figures 12, which develops a new optical effect in the case of illumination with white light 11, when the safety feature 16 is turned around the flip axis 41 parallel to the coordinate axis and. The safety feature 16 comprises the first triangular surface part 14, which is arranged in the second rectangular surface part 13. In the first surface part 14 the diffraction structure S (x, y) is distinguished because the spatial frequency f of the relief profile R (x, y) in the direction of the coordinate axis x within each period of the function of superposition M (x, y) is modified gradually or continuously over a predetermined spatial frequency range f, with the spatial frequency fi on the ith partial surface 47 (Figure 7) exceeding the spatial frequency fi-1 in the (i-1) -th previous partial surface 47. Therefore, in each period the first partial surface 47 has the spatial frequency f with the value fA. For the partial surface 47 in the period minimum, the spatial frequency is f = fM and for the partial surface 47 located at the end of the period, the value of the spatial frequency is f = fE, where fA <fM <fE, where  f = fE - fA. In the second surface part 13 the diffraction structure S (x, y) is distinguished because the spatial frequency f of the relief profile R (x, y) in the direction of the coordinate axis x within a period of the function of Overlap M (x, y) is reduced gradually or continuously from one partial surface 47 to the next. In one embodiment, the diffraction structure S ** (x, y) = R (-x, y) + M (-x, y) of the second surface part 13 is as an example the diffraction structure S (x, y) reflected in the plane defined by the coordinate axes y, z of the first surface part 14. The grid vectors and the mark 36 (figure 11) of the diffraction plane 20 (figure 9) are aligned in the two parts of surface 13, 14 essentially parallel to the turning axis 41. Gradient 38 is essentially parallel to the plane defined by the x and z coordinate axes.

In figure 12a, the safety feature 16 is in the x - y plane defined by the x and y coordinate axes, forming the observation direction 39 (figure 5) with the x coordinate axis at a right angle. In the case of white light 11 that has a perpendicular impact (Figure 1), the partial surfaces 47 light up in the area of the minimum of the overlapping function M (x, y). Since these partial surfaces 47 in both diffraction structures S (x, y), S ** (x, y) have the same raised profile R (x, y) and the same inclination  ≈ 0 °, the light rays 34 diffracted in the observation direction 39 to the two surface portions 13, 14 (figure 5) come from the same area of the visible spectrum, for example green so that the color contrast in the safety feature 16 between the first disappears surface part 14 and the second surface part 13. In the case of flipping of the safety feature 16 around the turning axis 41 the color contrast clearly appears with the increasing turning angle, as shown in Figure 12b . In the case of turning to the left, the color of the first surface part 14 shifts in the direction of red, since partial surfaces 47 (Figure 11) are effective with the raised profiles R (x, y), in which the spatial frequency f is less than fM. The color of the second surface part 13 shifts in the direction of the blue, since partial surfaces 47 are effective, in which the spatial frequency f of the raised profile R (x, y) is greater than fM. In figure 12c the safety feature 1 of the stratum shown in figure 12a is turned to the right around the turning axis 41. Also in the case of turning to the right the color contrast clearly appears, however with changed colors. The color of the first surface part 14 shifts in the direction of blue, since partial surfaces 47 are effective, in which the spatial frequency f of the raised profile R (x, y) is greater than the fM value, while that the color of the second surface part 13 shifts in the direction of red, since partial surfaces 47 are effective (figure 11), in which the spatial frequency f of the relief profile R (x, y) of the diffraction structure S ** (x, y) decreases compared to the fM value.

In another embodiment of the diffraction structure S (x, y) of Figure 11, the relief profile R (x, y) has on the partial surfaces 47 of each 1 / Fx period the same spatial frequency f, however the Relief profile R (x, y) differs between partial surfaces 47 by its azimuth angle φ of the grid vector in relation to the coordinate axis y. Within a period 1 / Fx, the azimuth angle modifica is modified gradually or continuously, for example in the range of  =  40º with  0º in the minimum of each period. The azimuth angle  is selected depending on the local inclination  (figure 5) of the average surface 33 (figure 5) in the interval  so that on the one hand the diffraction structure S (x, y) of the first part of surface 14 (figure 12a) emits light rays 34 (figure 5) of the predetermined color zone by means of the spatial frequency f, diffracted at all turning angles around the turning axis 41 (figure 12b, c) and on the other hand, the second surface part 13 (figure 12a), on which the reflected diffraction structure S ** (x, y) is molded, flashes only under a single predetermined turning angle in the predetermined color, for example in a mixed color generated by the green zone. At other turning angles, the second surface part 13 is dark gray. For the azimuth angle range  =  20 ° mentioned in this case by way of example, the green zone extends from the wavelength  = 530 nm (  0 °) to the wavelength  = 564 nm.

In Figure 13, the overlapping function M (x, y) used in the diffraction structure S (x, y) is an asymmetric function in the direction of the coordinate axis x. The overlapping function M (x, y) increases periodically within the period 1 / Fx from a minimum value to a maximum value, for example as the function y = const • x1.5. The spatial frequency Fx or Fy is in the range from 2.5 lines / mm to and with 10 lines / mm. Discontinuous sites that are produced by the H-path module operation are not shown (Figure 7). The "anisotropic" matte structure described above with the preferred direction essentially parallel to the x-axis coordinates is used as the relief profile R (x, y). Therefore, the incident light 11 (Figure 5) is dispersed in the form

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of fan mainly parallel to the coordinate axis and. The diffraction structure S (x, y) = R (x, y) + M (x, y) is molded in the first surface part 14 (figure 12a) and in the second surface part 13 (figure 12a) it is molded the diffraction structure S ** (x, y) = R (-x, y) + M (-x, y). By means of figure 12a, the optical effect of the safety feature 16 is clarified in the case of the light 11 that perpendicularly affects the x-y plane (figure 9). If the safety feature 16 is in the x - y plane, the incident light 11 is dispersed more intensely from the matte structure in the minimum range of the overlay function M (x, y), it must be set aside. the dispersion effect of the remaining surface portions 47 of the diffraction structures S (x, y), S ** (x, y). The backscattered light 11 from the surface parts 13, 14 has the color of the incident light 11 (Figure 5) and has on both surface parts 13, 14 the same surface brightness, so that no contrast between the two can be identified surface parts 13, 14. In Figure 12b, the incident light 11 (Figure 5) under an angle of incidence α intersects with the safety feature 16, which is turned to the left around the turning axis 41. Only In the second surface part 13 the incident light 11 is dispersed (Figure 5). In this lighting condition, the surface luminosity of the first surface part 14 is of smaller dimensions than in the second surface part 13, so that the first surface part 14 stands out as a dark surface in front of the second surface part 13 clear. In Figure 12c, the safety feature 16 does not turn to the right, the surface luminosities of the two surface parts 13, 14 being reversed.

In figures 12a to 12c, instead of a single first triangular surface part 14, a plurality of the first surface parts 14, which form a logo, a character, etc., could be arranged on the second surface part 13.

In another additional embodiment, instead of simple mathematical functions, relief images, such as coins and medals, are also used as overlapping function M (x, y) at least partially continuous in the diffraction structure S ( x, y), the relief profile being R (x, y) advantageously being a "isotropic" matte structure. The observer of the security element 2 in this embodiment obtains the effect of a three-dimensional image with a characteristic surface structure. In the rotation and turning of the security element 2, the distribution of brightness in the image is modified correspondingly to the expectation in case of an authentic relief image, however the projecting elements do not cast any shadow.

Without departing from the idea of the invention, all diffraction structures S are limited in their structure height by the value HSt (Figure 1), as demonstrated by Figure 7. The overlapping functions M (x, y) and the relief profiles R (x, y) used in the special embodiments described above may be arbitrarily combined with other diffraction structures S (x, y).

The use of security features 16 described above in security element 2 has the advantage that security feature 16 forms an effective barrier against attempts to holographically reproduce security element 2. In a holographic copy, the characteristics of the stratum shifts or color shifts on the surface of security feature 16 only in a modified manner.

Claims (15)

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one.

Safety element (2) of a stratified composite material (1) with microscopically thin optically active structures (9) of a surface pattern (12) included between transparent layers (4, 5; 6) of the laminated composite material (1), the optically active structures (9) being molded into surface portions (13; 14; 15; 46) of a safety feature (16) in a plane defined by the coordinate axes (x; y) of the surface pattern (12 ) on a boundary surface (8) reflecting between the layers (5; 6), characterized in that at least a part of the surface (13; 14; 15) with dimensions greater than 0.4 mm has a diffraction structure (S; S *; S **) formed by an additive or subtractive overlay of an overlay function (M) that describes a macroscopic structure with a macroscopically thin profile (R), the overlay function (M) being the profile in relief (R) and diffraction structure (S ; S *; S **) coordinate functions (x; and) and describing the relief profile (R) an optically active structure (9) that disperses light, which preserves the predetermined relief profile (R) following the overlapping function (M), and why an average surface (33) defined by the at least partially continuous overlapping function (M), it is curved at least in partial areas and has a predetermined local inclination angle () at each point by the overlapping function gradient (M), it is no function rectangular or triangular periodically and is slowly modified compared to the relief profile (R).

2.

Safety element (2) according to claim 1, characterized in that the overlapping function (M) is a partially continuous periodic function with a spatial frequency (F) of at most 20 lines / mm.

3.

Safety element (2) according to claim 1, characterized in that the overlay function (M) is a periodic, partially continuous, asymmetric function with a spatial frequency (F) in the range of 2.5 lines / mm to 10 lines / mm

Four.

Safety element (2) according to claim 1, characterized in that adjacent extreme values of the overlapping function (M) are spaced apart from each other on the surface part (13, 14, 15) by at least 0.025 mm.

5.

Security element (2) according to one of claims 2 to 4, characterized in that the relief profile (R) is a matt anisotropic structure having a preferred direction with an azimuthal angle ().

6.

Security element (2) according to claim 5, characterized in that the security feature (16; 16 ’) has at least two adjacent surface parts (13; 14; 15) and that in the first surface part

(14) the first diffraction structure (S) is molded and in the second surface part (13; 15) the second diffraction structure (S *; S **) differs from the first diffraction structure (S), the preferred direction of the first relief profile (R) being aligned on the first surface part (14) and the preferred direction of the second relief profile (R) on the second surface part (13; 15) essentially in parallel.

7.

Security element (2) according to one of claims 5 to 6, characterized in that in the diffraction structure (S; S *; S **) the preferred direction of the relief profile (R) is essentially parallel to a gradient plane that is determined by the gradient (38) of the superposition function (M) and a normal surface (21) that is perpendicular to the surface of the stratified composite (1).

8.

Safety element (2) according to one of claims 5 to 7, characterized in that the first diffraction structure (S) is formed on a first surface part (14) that is formed as the sum of the relief profile (R) and the overlapping function (M), and because on a second surface part (13; 15) the second diffraction structure (S *) is molded which forms as the difference (R-M) of the same embossed profile (R) and the same overlay function (M).

9.

Security element (2) according to one of claims 5 to 8, characterized in that in the diffraction structure (S; S *; S **) the preferred direction of the relief profile (R) is essentially perpendicular to a plane in gradient that is determined by the gradient (38) of the superposition function (M) and a normal surface (21) that is perpendicular to the surface of the laminated composite 1.

10.

Security element (2) according to claim 5, characterized in that in the first surface part

(14) the first diffraction structure (S) is formed from the sum of the relief profile (R) and the overlay function (M), and because in the second surface part (13; 15) the structure Overlay (S **) is the first diffraction structure (S) reflected in the plane of the surface pattern (12).

eleven.

 Security element (2) according to claim 1, characterized in that the relief profile (R) is an isotropic matte structure.

12.

Security element (2) according to claim 11, characterized in that the overlay function (M) describes a relief image.

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13.

Safety element (2) according to claim 11, characterized in that the overlay function (M) describes a spherical shell.

14.

Security element (2) according to one of claims 1 to 13, characterized in that

Additional surface (17; 18; 19) with the optically active structures (9) are parts of the surface pattern (12) and because at least one of the surface elements (17; 18; 19) limits the characteristic of security (16). 15. Security element (2) according to one of claims 1 to 14, characterized in that at least one identification mark (37) with an optically active structure (9) that differs from the diffraction structure (S; 10 S *; S **) is arranged in at least one of the surface parts (13; 14; 15) and why the identification mark (37) used as a reference for the orientation of the stratified composite material (1) has one of the optically active structures (9) of the group of diffractive or light scattering structures or a reflective surface. 12